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Page 1: RXTE Studies of Accreting X-ray Pulsars via Cyclotron Lines

RXTE Studies of Accreting X-ray Pulsars via Cyclotron Lines

Rick Rothschild on behalf of the MAGNET collaboration

• RXTE has doubled the number of known cyclotron lines sources

• RXTE has observed multiple line sources in outburst

• RXTE has provided multiple visits to both persistent and transient sources to allowluminosity-dependent effects to be investigated

• Spin phase resolved spectroscopy has allowed for probing different portions of the scattering region as the neutron star rotates.

• RXTE has revealed variations with pulse shape.

Heindl et al. 2003

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The Numbers:

68 accreting X-ray pulsars25 Be binaries 6 Possible Be binaries14 Supergiants10 Symbiotics binaries3 Low mass X-ray Binaries1 High Mass X-ray binary 1 Intermediate mass (Her X-1)1 Possible white dwarf7 Unknown Companion

17 Sources exhibiting one or more cyclotron lines

9 Be binaries5 Supergiants1 Intermediate mass1 Symbiotic binary (New)1 Possible white dwarf

5 Sources possibly having a line3 Be binaries1 Supergiant1 Unknown

Caballero et al. 2010, 2011

A0535+26

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RXTE Observations of Cyclotron Line Variability with Luminosity

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Theory: Emission Geometry

Critical Luminosity for Bimodal Spectral Variabilityin Accretion-Powered X-Ray Pulsars

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Theory: Variation of CRSF Energy

Critical Luminosity for Bimodal Spectral Variabilityin Accretion-Powered X-Ray Pulsars

• We see 4 distinct types of variation of Ecyc with variation of Lx

Supercritical,radiationdeceleration

Lx

Subcritical,Coulomb stopping

Subcritical,gas-shock

Subcritical,direct impact

Ecyc

Ecyc = E*

Lx

Region of Interest

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Theory: Variation of Emission Height

Critical Luminosity for Bimodal Spectral Variabilityin Accretion-Powered X-Ray Pulsars

• The observations of Ecyc imply 4 distinct types of variation of the characteristic emission height h with variation of Lx

Supercritical,radiationdeceleration

Lx

h

Subcritical,Coulomb stopping

Subcritical,gas-shock

Subcritical,direct impact

h = 0

Lx

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Advances in Understanding Cyclotron Lines from a Physics Point of View

Predicted cyclotron line shapes on top of a Fermi-Dirac continuum model with Ecut=10 keV and Efold=12 keV. Modeled is a cylindrical column with B/Bcrit = 0.05, kTe = 3 keV, τes = 10-3. Note Bcrit = 4.4 x 1013 Gauss

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Combining the Continuum and Cyclotron Line Modeling

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Her X-1, the Original Cyclotron Line Source

Trümper et al. 1977

35 day super modulation

1.24 s pulsed flux

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The evolution of the pulse profile is intimately linked to the evolution of the 35 day Main-On.

The left shoulder goes away as the Main-On progresses.

Klochkov & Staubert

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Variation of Power Law Photon Index with Pulse Phase and Main-On Interval

The power law photon index softens slightly with pulse phase as the pulse profile varies throughout the 35 day Main-ON, with two EXCEPTIONS:

1) Phase ~0.6: Abrupt change in index lessens as the left shoulder of the profile diminishes.

2) Phase ~0.7-0.9: The index flattens from 0.7-0.8 and steepens again from 0.8-0.9

Is this Steve Pravdo’s viewing down the pole towards us and the gravitationally beamed pole on the back side?

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While the power law photon index varies with pulse shape in the Main-On, the cyclotron line variation is essentially the same throughout the Main-On

Thus our view of the cyclotron resonant scattering region is unchanged throughout the 35-day Main-On, but the continuum emission region is affected.

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Variation of the Cyclotron Line with 35 Day Phase

Behavior is the same for different 35 Day Main-On’s:

Apparent slow rise in centroid energy and then abrupt decrease.

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What is the long term cyclotron line variation in Her X-1 telling us?

• The abrupt change in the 1980’s

• The slow decrease since the 1990’s

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Variation of Her X-1 Cyclotron Line Energy with Mean Main-On Flux

Staubert & Klochkov

Red Points are Post-2006

Black Points are Pre-2006

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Variation of Cyclotron Energy with Average Main-On Flux

This works well until about 2007, then another possible abrupt change occurs or the relationship no longer holds.

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Luminosity (i.e. ASM Main-On Maximum) Corrected Cyclotron Line Energies up to ~2007, and uncorrected after that.

Yet again, Her X-1 is presenting us with surprises and challenges to our understanding of magnetic poles of neutron stars.

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Thank you to everyone who made RXTE a big success.

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Present List of Cyclotron Line Sources

Possible new cyclotron line source: IGR J18179-1621 with 11.8 s period and Ecyc~21 keV

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Becker & Wolff (2007) and subsequent work by Becker and his students are developing a bulk Comptonization model of accretion onto the magnetic poles.

Eventually this physics-based treatment will replace empirical modeling of accretion powered pulsar spectra.

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